360 Renormalization Group Equations for Quantum Gravity Based on the Discrete Parent Group

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2026/05/28
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9 mins read


 

Renormalization Group Equations for Quantum Gravity Based on the Discrete Parent Group

Author: Suhang Zhang, Luoyang, Henan

Abstract

The ultraviolet divergences in quantum gravity originate from the assumption of infinitely differentiable continuous spacetime adopted by conventional renormalization group theory. Breaking away from the continuous manifold framework, this paper reconstructs renormalization group theory based on the fundamental elements, recursive hierarchy and dynamic curvature of the Global Discrete Parent Group (Zhang Group). We define discrete coarse-graining transformations (fundamental element merging and hierarchy transition) and refinement transformations (fundamental element splitting and hierarchy descent), and derive hybrid discrete-continuous renormalization group flow equations. The equations take distinct forms in three regimes: the deep discrete regime at the Planck scale is free of ultraviolet divergences; the transition regime dominated by hybrid groups yields coupled discrete-continuous equations; under the threefold limit (low curvature, single hierarchy and full coarse-graining), the system reduces to conventional continuous renormalization group equations. This framework fundamentally eliminates ultraviolet divergences, provides a self-consistent renormalization scheme for quantum gravity, and presents testable physical implications.

Keywords: Zhang Group; Quantum Gravity; Renormalization Group; Ultraviolet Divergence; Discrete Parent Group; Recursive Hierarchy

1. Introduction

1.1 Dilemmas of Conventional Renormalization Group

As a core tool of quantum field theory, the Renormalization Group (RG) has successfully resolved ultraviolet divergences in Quantum Electrodynamics and Quantum Chromodynamics. Nevertheless, its application to quantum gravity encounters fundamental obstacles:

Problem Description
Non-renormalizability The gravitational coupling constant of the Einstein–Hilbert action carries a negative mass dimension, leading to uncontrollable growth of divergences with perturbation order.
Reliance on continuous assumption Conventional RG is formulated on continuous spacetime and infinitely differentiable manifolds, which conflicts with the discrete nature expected for quantum gravity.
Background dependence Traditional RG relies on a fixed background spacetime, contradicting the background independence of general relativity.
Absence of ultraviolet fixed points The asymptotic safety conjecture postulates the existence of non-Gaussian fixed points, yet such points cannot be derived from first principles.

All the above issues stem from a universal premise: conventional RG assumes spacetime remains continuous down to arbitrarily small scales.

1.2 Methodology of the Discrete Parent Group Framework

Based on the theory of the Global Discrete Parent Group (G_Z, Zhang Group), this work puts forward the following proposition:

Spacetime possesses a minimum scale of discrete fundamental elements. Renormalization transformations are essentially the merging or splitting of discrete elements and transitions between recursive hierarchies, rather than pure continuous scale scaling. This intrinsic discreteness cuts off ultraviolet divergences at the root.

Core insights:

- Ultraviolet divergences arise from the mathematical assumption that the integral upper limit satisfies k \to \infty.
- Within the Zhang Group framework, there exists a minimum discrete scale a_{\min} \sim \ell_\text{P}, which naturally sets an upper cutoff k_{\max} \sim 1/a_{\min}.
- Scale transformations are not continuous scaling operations but discrete jumps between hierarchies.

1.3 Paper Organization

Section 2 establishes basic variables within the Zhang Group framework. Section 3 defines discrete coarse-graining and refinement transformations. Section 4 derives discrete renormalization group flow equations. Section 5 discusses the adaptation to quantum gravity and the elimination of divergences. Section 6 presents physical predictions and experimental schemes. Section 7 draws conclusions.

2. Basic Setup: Renormalization Variables under the Zhang Group

2.1 Structural Variables of Spacetime

Spacetime is characterized by the following variables in the Zhang Group framework:

Variable Symbol Domain Physical Meaning
Discrete element scale     Characteristic scale of the fundamental spacetime units
Recursive hierarchy     Current depth of the observed recursive structure
Spacetime curvature     Local geometric curvature (positive or negative)
Gauge coupling constants     Coupling strengths of fundamental interactions
Gravitational coupling constant     Newton’s gravitational constant (may run with scale)

2.2 Three Characteristic Regimes

The system is divided into three distinct regimes according to variable combinations:

Regime Conditions Description
Deep Discrete Regime   Pure discrete structure; continuous approximation completely breaks down
Transition Regime               Dominated by hybrid discrete-continuous groups
Continuous Regime   Continuous Lie group approximation is valid under the threefold limit

2.3 Review of the Threefold Limit

The threefold limit \mathcal{L} is defined as:

\mathcal{L}:
\begin{cases}
n = N_{\max} \quad (\text{Single recursive hierarchy})\\
R \to 0 \quad (\text{Zero curvature limit})\\
a \to 0,\ \epsilon \to 0 \quad (\text{Full coarse-graining limit})
\end{cases}


Important Clarification: Physically, a cannot be smaller than the Planck length \ell_\text{P}. The limit a \to 0 is only an effective approximation describing the regime where discrete effects are negligible.

3. Discrete Coarse-Graining and Refinement Transformations

3.1 Coarse-Graining Transformation (Scale Increasing)

Define the coarse-graining operation \mathcal{C}: (a, n) \to (a', n'):

\mathcal{C}:
\begin{cases}
a' = \kappa \cdot a,\quad \kappa > 1\\
n' = n + 1\\
\text{Number of merged fundamental elements} = \kappa^d
\end{cases}


where d denotes spacetime dimension and \kappa is the coarse-graining factor (typically \kappa=2).

Symmetry of the Zhang Group imposes the constraint during coarse-graining:

\forall\, g \in G_Z,\quad \mathcal{C}(g \cdot \phi) = \mathcal{C}(g) \cdot \mathcal{C}(\phi) + \mathcal{O}(a^2)


namely, the coarse-graining map approximately commutes with group actions.

3.2 Refinement Transformation (Scale Decreasing)

The refinement operation \mathcal{F} is the inverse of coarse-graining:

\mathcal{F}:
\begin{cases}
a' = a / \kappa,\quad \kappa > 1\\
n' = n - 1\\
\text{Number of split fundamental elements} = \kappa^d
\end{cases}


Refinement is bounded by the minimum scale a_{\min} = \ell_\text{P}. The operation \mathcal{F} is no longer well-defined when a = \ell_\text{P}, which gives rise to a natural ultraviolet cutoff.

3.3 Group Invariance Constraints

Coarse-graining and refinement must preserve the fundamental symmetries of the Zhang Group, subject to constraints from the Geometric Recursive Conservation Law (GPCL):

\frac{d}{d\ln a} \big(\text{Conserved Quantity}\big) = 0 \quad (\text{up to hierarchy corrections})


For the action functional S:

S[\mathcal{C}(\phi)] = S[\phi] + \Delta S_\text{level} + \Delta S_\text{curvature} + \Delta S_\text{discrete}


All correction terms vanish under the threefold limit \mathcal{L}.

4. Discrete Renormalization Group Flow Equations

4.1 General Form of Flow Equations

Introduce the scale parameter t = \ln(a/a_{\min}), where t=0 corresponds to the Planck scale and t \to \infty corresponds to macroscopic scales.

Theorem 1 (Discrete RG Equation): Within the Zhang Group framework, the evolution of coupling constants with scale satisfies:

\frac{dg_i}{dt} = \beta_i^\text{(cont)}(g) + \beta_i^\text{(disc)}(g, a, n, R) + \beta_i^\text{(level)}(g, n)


- \beta_i^\text{(cont)}(g): Conventional continuous contribution originating from loop diagrams
- \beta_i^\text{(disc)}(g, a, n, R): Discrete correction term, dependent on a, n and R
- \beta_i^\text{(level)}(g, n): Hierarchy transition term, activated during changes of recursive level

4.2 Reduced Forms in Three Regimes

4.2.1 Deep Discrete Regime (t \approx 0,\ n=0,\ R \gg R_c)

Discrete effects dominate, and continuous contributions are negligible:

\frac{dg_i}{dt} = \beta_i^\text{(disc)} + \beta_i^\text{(level)}


Key feature: No ultraviolet divergences. The integral upper limit is naturally bounded by k_{\max} \sim 1/a_{\min}, and continuous integrals are replaced by finite discrete summations, which regularize all divergences.

4.2.2 Transition Regime (0 < t < T_\text{mix},\ 1 \le n \le N_{\max}-1,\ R \sim R_c)

Discrete and continuous contributions are comparable:

\frac{dg_i}{dt} = \beta_i^\text{(cont)} + \beta_i^\text{(disc)} + \beta_i^\text{(level)}


When the recursive level increases, the system evolves from the deep discrete regime toward the continuous regime. The hierarchy term induces a finite jump in coupling constants:

\left.\Delta g_i\right|_{n \to n+1} = \gamma_i \cdot \frac{a^2}{a_{\min}^2} + \mathcal{O}(a^4)


4.2.3 Continuous Regime (t \to \infty,\ n = N_{\max},\ R \to 0)

Under the threefold limit, discrete and hierarchy corrections vanish:

\frac{dg_i}{dt} = \beta_i^\text{(cont)}(g)


This recovers the conventional continuous renormalization group equation adopted in the Standard Model.

4.3 Explicit Example: Simplest Model

For illustrative purposes, we present the discrete RG equation for a minimal scalar field model (full derivation in the appendix):

\frac{dg}{dt} = \frac{b_0}{(4\pi)^2} g^3 + \frac{b_1}{(4\pi)^4} g^5 + \cdots + \lambda \cdot \frac{a^2}{a_{\min}^2} \cdot g \cdot \cos\left(\frac{R}{R_c}\right) + \mu \cdot e^{-n} \cdot g^2


- The first two terms are conventional continuous beta functions (b_0, b_1 > 0)
- The third term denotes discrete corrections, which become prominent near a = a_{\min}
- The fourth term is the hierarchy decay term, decaying exponentially with increasing n

\boxed{\lim\limits_{a \to 0,\ n \to \infty,\ R \to 0} \frac{dg}{dt} = \frac{b_0}{(4\pi)^2} g^3 + \frac{b_1}{(4\pi)^4} g^5 + \cdots}


The equation reduces to the traditional form under the threefold limit.

5. Adaptation to Quantum Gravity and Elimination of Divergences

5.1 Running of the Gravitational Coupling Constant

Let g_\text{grav} = G_N E^2 be the dimensionless gravitational coupling. Its evolution reads:

\frac{dg_\text{grav}}{dt} = 2g_\text{grav} + \beta_\text{grav}^\text{(loop)}(g_\text{grav}) + \beta_\text{grav}^\text{(disc)}(a, n, R)


- The term 2g_\text{grav} arises from the negative mass dimension of the gravitational coupling after dimensionless normalization
- \beta_\text{grav}^\text{(loop)} corresponds to higher-order loop contributions
- \beta_\text{grav}^\text{(disc)} stands for discrete corrections, which dominate near the Planck scale

5.2 Natural Ultraviolet Cutoff

Theorem 2 (Elimination of Ultraviolet Divergences): Within the Zhang Group framework, all loop integrals in quantum gravity are naturally cut off at k_{\max} = 1/a_{\min}.

Proof Sketch:

- Conventional continuous integral: \displaystyle\int_0^\Lambda d^4k\,f(k) diverges as \Lambda \to \infty.
- Discrete summation in the present framework: \displaystyle\sum\limits_{k} \Delta^4 k\,f(k), where momentum takes discrete values with a finite upper bound k_{\max} \sim 1/a_{\min}.
Since a_{\min} = \ell_\text{P} is a finite constant, all summations are finite and divergences are completely removed.

5.3 Comparison with Conventional Renormalization Group

Aspect Conventional Continuous RG Discrete RG in This Framework
Spacetime structure Continuous manifold Discrete fundamental elements + recursive hierarchy
Scale transformation Continuous scaling Discrete merging/splitting + hierarchy transition
Ultraviolet behavior Divergences exist and require artificial regularization Natural cutoff, no divergences
Fixed points Reliant on conjectures (asymptotic safety) Derived intrinsically from discrete structure
Continuous limit Fundamental postulate Emergent result under the threefold limit

The conventional renormalization group is recovered as a special case of the present framework under the threefold limit.

6. Physical Predictions and Experimental Schemes

6.1 Prediction 1: High-Energy Behavior of Gravitational Coupling

The framework predicts that when the energy approaches the Planck scale (E \sim E_\text{P}, i.e. a \sim \ell_\text{P}), discrete corrections dominate, and the gravitational coupling no longer evolves monotonously but exhibits oscillatory decay:

g_\text{grav}(E) \sim \frac{1}{\ln(E/E_\text{P})} \cdot \cos\left(\frac{E_\text{P}}{E}\right), \quad E \to E_\text{P}


This behavior differs from both asymptotic safety (monotonic convergence to a fixed point) and asymptotic freedom (monotonic decay to zero), and is experimentally distinguishable.

6.2 Prediction 2: Discrete Structure of Energy Spectra

For processes beyond the threshold energy E_\text{th} \sim 10^{18}\ \text{GeV}:

- Distinct discrete peaks emerge in particle energy spectra
- The peak spacing is determined by the minimum discrete scale: \Delta E \sim \hbar c / a_{\min} \sim E_\text{P}

Such features may be observed in ultrahigh-energy cosmic ray spectra and extreme astrophysical events.

6.3 Prediction 3: Physical Signals of Hierarchy Transitions

Finite jumps of physical parameters occur during transitions between recursive hierarchies (e.g. n=1 \to n=2):

- Coupling constants and particle masses undergo finite discontinuities at transition points
- The jump amplitude is correlated with spacetime curvature: \Delta g \sim (R/R_c)^2

This effect may leave observable imprints in early universe phase transitions and black hole accretion disk phenomena.

6.4 Feasibility of Experimental Tests

Prediction Energy Scale Detection Method Estimated Time Scale
Oscillation of gravitational coupling   Cosmic microwave background, gravitational wave background 10–20 years
Discrete peaks in energy spectra   Ultrahigh-energy cosmic rays, gamma-ray bursts 15–25 years
Hierarchy transition signals Variable Early universe phase transitions, black hole physics 5–15 years

7. Conclusions

1. Novel Renormalization Group Framework: Based on the Global Discrete Parent Group, we define discrete coarse-graining and refinement transformations, and derive hybrid discrete-continuous renormalization group flow equations.
2. Removal of Ultraviolet Divergences: The minimum discrete scale of spacetime a_{\min} = \ell_\text{P} acts as a natural ultraviolet cutoff, resolving the ultraviolet divergence problem of quantum gravity at the fundamental level.
3. Conventional RG as a Special Case: Under the threefold limit (single hierarchy, zero curvature and full coarse-graining), the discrete RG equations reduce to standard continuous renormalization group equations.
4. Testable Predictions: The framework puts forward unique predictions including oscillatory behavior of gravitational coupling at high energy, discrete spectral peaks and parameter jumps across hierarchies, which can be verified by future observations and experiments.
5. Future Work: Complete full one-loop calculations for discrete RG equations; perform quantitative comparisons with asymptotic safety and loop quantum gravity; extend the framework to full particle physics models containing fermions and gauge fields.

References

[1] Zhang S H. Proof that Continuous Lie Groups are Special Cases of Discrete Groups from the Perspective of Recursive Geometry[J]. Mathematical Physics Preprint, 2026.

[2] Zhang S H. Embedding Mapping Derivation of U(1)\times SU(2)\times SU(3) Gauge Group within the Global Discrete Parent Group (Zhang Group)[J]. Mathematical Physics Preprint, 2026.

[3] Zhang S H. Discrete Order Geometry and Multi-Origin Recursive Geometry — The Underlying Spacetime Structure of Universal Recursive Systems[J]. Unpublished Academic Paper, 2026.

[4] Zhang S H. Geometric Recursive Conservation Law System: Reconstruction and Generalization of Classical Group Symmetry Theory[J]. Mathematical Physics Preprint, 2026.

[5] Wilson K G. Renormalization group and critical phenomena[J]. Physical Review B, 1971, 4(9): 3174.

[6] Weinberg S. Ultraviolet divergences in quantum theories of gravitation[M]//General Relativity: An Einstein Centenary Survey. Cambridge University Press, 1979: 790-831.

[7] Reuter M. Nonperturbative evolution equation for quantum gravity[J]. Physical Review D, 1998, 57(2): 971.

[8] Rovelli C. Loop quantum gravity[J]. Living Reviews in Relativity, 1998, 1(1): 1.

[9] 't Hooft G. Dimensional regularization and the renormalization group[J]. Nuclear Physics B, 1973, 61: 455-468.

 


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